Chapter 7: The Laplace Transform Department of Electrical - - PowerPoint PPT Presentation

Laplace and Inverse Laplace Transform: Definitions and Basics

Chapter 7: The Laplace Transform

王奕翔

Department of Electrical Engineering National Taiwan University ihwang@ntu.edu.tw

November 18, 2013

1 / 19 王奕翔 DE Lecture 10

Laplace and Inverse Laplace Transform: Definitions and Basics

Solving an initial value problem associated with a linear differential equation:

1 General solution = complimentary solution + particular solution. 2 Plug in the initial conditions to specify the undetermined coefficients.

Question: Is there a faster way?

2 / 19 王奕翔 DE Lecture 10

Laplace and Inverse Laplace Transform: Definitions and Basics

In Chapter 4, 5, and 6, we majorly deal with linear differential equations with continuous, differentiable, or analytic coefficients. But in real applications, sometimes this is not true. For example: E(t) L C R E(t) t Square voltage input: Periodic, Discontinuous. Question: How to solve the current? How to deal with discontinuity?

3 / 19 王奕翔 DE Lecture 10

Laplace and Inverse Laplace Transform: Definitions and Basics

In this lecture we introduce a powerful tool:

Laplace Transform

Invented by Pierre-Simon Laplace (1749 - 1827).

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Laplace and Inverse Laplace Transform: Definitions and Basics

Overview of the Method

Apply Laplace transform Apply inverse Laplace transform Find unknown y(t) that satisfies DE and initial conditions Transformed DE becomes an algebraic equation in Y(s) Solve transformed equation for Y(s) Solution y(t)

• f original IVP

−1

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Laplace and Inverse Laplace Transform: Definitions and Basics

1 Laplace and Inverse Laplace Transform: Definitions and Basics

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Laplace and Inverse Laplace Transform: Definitions and Basics

Definition of the Laplace Transform

Definition For a function f(t) defined for t ≥ 0, its Laplace Transfrom is defined as F(s) := L {f(t)} := ∫ ∞ e−stf(t)dt, given that the improper integral converges. Note: Use capital letters to denote transforms. f(t)

L

− → F(s), g(t)

L

− → G(s), y(t)

L

− → Y(s), etc. Note: The domain of the Laplace transform F(s) (that is, where the improper integral converges) depends on the function f(t)

7 / 19 王奕翔 DE Lecture 10

Laplace and Inverse Laplace Transform: Definitions and Basics

Examples of Laplace Transform

Example Evaluate L {1}. L {1} = ∫ ∞ e−st(1)dt = lim

T→∞

∫ T e−stdt = lim

T→∞

[−e−st s ]T = lim

T→∞

1 − e−sT s . When does the above converge? s > 0! Hence, the domain of L {1} is s > 0, and L {1} = 1 s .

8 / 19 王奕翔 DE Lecture 10

Laplace and Inverse Laplace Transform: Definitions and Basics

Examples of Laplace Transform

Example Evaluate L {t}. L {t} = ∫ ∞ te−stdt = lim

T→∞

∫ T td (−e−st s ) = lim

T→∞

[−te−st s ]T + ∫ T 1 s e−stdt = lim

T→∞

−Te−sT s + 1 s L {1} . When does the above converge? s > 0! Hence, the domain of L {t} is s > 0, and L {t} = 1 s2 .

9 / 19 王奕翔 DE Lecture 10

Laplace and Inverse Laplace Transform: Definitions and Basics

Laplace Transform of tn

L {tn} = n! sn+1 , n = 0, 1, 2, . . . , s > 0 Proof: One way is to prove it by induction. We will show another proof after discussing the Laplace transform of the derivative of a function.

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Laplace and Inverse Laplace Transform: Definitions and Basics

Laplace Transform of eat

L { eat} = 1 s − a, s > a Proof: L { eat} = ∫ ∞ eate−stdt = lim

T→∞

∫ T e−(s−a)tdt = lim

T→∞

[−e−(s−a)t s − a ]T = lim

T→∞

1 − e−(s−a)T s − a When does the above converge? s − a > 0! Hence, the domain of L {eat} is s > a, and L {eat} =

1 s−a.

11 / 19 王奕翔 DE Lecture 10

Laplace and Inverse Laplace Transform: Definitions and Basics

Laplace Transform of sin(kt) and cos(kt)

L {sin(kt)} = k s2 + k2 , L {cos(kt)} = s s2 + k2 , s > 0 Proof: L {sin(kt)} = ∫ ∞ sin(kt)e−stdt = ∫ ∞ sin(kt)d (−e−st s ) = [− sin(kt)e−st s ]∞ + k s ∫ ∞ cos(kt)e−stdt = [− sin(kt)e−st s ]∞ + k sL {cos(kt)} When does the above converge? s > 0! = ⇒ [

− sin(kt)e−st s

]∞

0 = 0

12 / 19 王奕翔 DE Lecture 10

Laplace and Inverse Laplace Transform: Definitions and Basics

Laplace Transform of sin(kt) and cos(kt)

L {sin(kt)} = k s2 + k2 , L {cos(kt)} = s s2 + k2 , s > 0 Proof: L {cos(kt)} = ∫ ∞ cos(kt)e−stdt = ∫ ∞ cos(kt)d (−e−st s ) = [− cos(kt)e−st s ]∞ − k s ∫ ∞ sin(kt)e−stdt = [− cos(kt)e−st s ]∞ − k sL {sin(kt)} When does the above converge? s > 0! = ⇒ [

− cos(kt)e−st s

]∞

0 = 1 s.

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Laplace and Inverse Laplace Transform: Definitions and Basics

Laplace Transform of sin(kt) and cos(kt)

L {sin(kt)} = k s2 + k2 , L {cos(kt)} = s s2 + k2 , s > 0 Proof: { L {sin(kt)} = k

sL {cos(kt)}

L {cos(kt)} = 1

s − k sL {sin(kt)}

Solve the above, we get the result: L {sin(kt)} = k sL {cos(kt)} = k s2 − k2 s2 L {sin(kt)} = ⇒ s2 + k2 s2 L {sin(kt)} = k s2 = ⇒ L {sin(kt)} = k s2 + k2 L {cos(kt)} = s kL {sin(kt)} = s s2 + k2 .

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Laplace and Inverse Laplace Transform: Definitions and Basics

Laplace Transform is Linear

Theorem For any α, β, f(t)

L

− → F(s), g(t)

L

− → G(s), L {αf(t) + βg(t)} = αF(s) + βG(s) Proof: It can be proved by the linearity of integral. Example Evaluate L {sinh(kt)} and L {cosh(kt)}. A: sinh(kt) = 1

2

( ekt − e−kt) , cosh(kt) = 1

2

( ekt + e−kt) . Hence sinh(kt)

L

− → 1 2 ( 1 s − k − 1 s + k ) = k s2 − k2 , s > |k| cosh(kt)

L

− → 1 2 ( 1 s − k + 1 s + k ) = s s2 − k2 , s > |k| .

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Laplace and Inverse Laplace Transform: Definitions and Basics

Laplace Transforms of Some Basic Functions

tn

L

− → n! sn+1 s > 0 eat

L

− → 1 s − a s > a sin(kt)

L

− → k s2 + k2 s > 0 cos(kt)

L

− → s s2 + k2 s > 0 sinh(kt)

L

− → k s2 − k2 s > |k| cosh(kt)

L

− → s s2 − k2 s > |k|

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Laplace and Inverse Laplace Transform: Definitions and Basics

Existence of Laplace Transform

Theorem (Sufficient Conditions for the Existence of Laplace Transform) If a function f(t) is piecewise continuous on [0, ∞), and

• f exponential order,

then L {f(t)} exists for s > c for some constant c. Definition A function f(t) is of exponential order if ∃ c ∈ R, M > 0, τ > 0 such that |f(t)| < Mect, ∀ t > τ. Note: If f(t) is of exponential order, then ∃ c ∈ R such that for s > c, lim

t→∞ f(t)e−st = 0.

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Laplace and Inverse Laplace Transform: Definitions and Basics

Existence of Laplace Transform

Theorem (Sufficient Conditions for the Existence of Laplace Transform) If a function f(t) is piecewise continuous on [0, ∞), and

• f exponential order,

then L {f(t)} exists for s > c for some constant c. Proof: For sufficiently large T > τ, we split the following integral: ∫ T f(t)dt = ∫ τ f(t)e−stdt

• I1

+ ∫ T

τ

f(t)e−stdt

• I2

. We only need to prove that I2 converges as T → ∞: |I2| ≤ ∫ T

τ

|f(t)e−st|dt = ∫ T

τ

|f(t)|e−stdt ≤ ∫ T

τ

Mecte−stdt, which converges as T → ∞ for s > c since L { ect} exists.

18 / 19 王奕翔 DE Lecture 10

Laplace and Inverse Laplace Transform: Definitions and Basics

In this lecture, we focus on functions that are piecewise continuous on [0, ∞), and

• f exponential order

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